Problem 1: Symmetries of Newton's Laws In this problem, we will use the short-hand R(0) (sin θ co...
(b) Waves appear in a wide variety of physical systems and are described by the equation where ▽·▽ = ▽2 is the Laplacian and c* is the speed of propagation. List all of the symmetries of this equation. (c) Suppose we change the wave equation to the following Which symmetries from part (b) are no longer symmetries when y 0. (d) When γ > 0, we would usually say that the wave is dissipating energy. Show this explicitly by finding...
(15 points) Encounter with a semi-infinite potential "well" In this problem we will investigate one situation involving a a semi-infinite one-dimensional po- tential well (Figure 1) U=0 region 1 region 2 region 3 Figure 1: Semi-infinite potential for Problem 3 This potential is piecewise defined as follows where Uo is some positive value of energy. The three intervals in x have been labeled region 1,2 and 3 in Figure 1 Consider a particle of mass m f 0 moving in...
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Problem 3: Use simple kinetic theory of gases discussed in section 1.3.2 as well as Fourer's law of condustion to prove: 2 R373 D11 = 3113/202pm Dal We were unable to transcribe this imageof a nes. the xed the led negligible The following assumptions about the structure of the cases are made in order to investigate the statistical rules of the random motion of the molecules: The size of the gas molecules is negligible compared with the distance...